2006
DOI: 10.1088/1475-7516/2006/08/006
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Curvature perturbation from symmetry breaking the end of inflation

Abstract: We consider a two-field hybrid inflation model, in which the curvature perturbation is predominantly generated at the end of inflation. By finely tuning the coupling of the fields to the waterfall we find that we can get a measurable amount of non-gaussianity.

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Cited by 76 publications
(109 citation statements)
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“…Typically, we will also find that the sourcing of curvature modes by isocurvature modes will be moderate, although this is not required; rather, weak sourcing (sin ∆ N ≪ 1) or strong sourcing (cos ∆ N ≪ 1) simply makes the bound in equation (60) even that much harder to satisfy. In other words, searching for scenarios where the sourcing is moderate maximizes the chance of finding scenarios that produce large non-Gaussianity.…”
Section: Conditions For Large |Fnl|mentioning
confidence: 97%
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“…Typically, we will also find that the sourcing of curvature modes by isocurvature modes will be moderate, although this is not required; rather, weak sourcing (sin ∆ N ≪ 1) or strong sourcing (cos ∆ N ≪ 1) simply makes the bound in equation (60) even that much harder to satisfy. In other words, searching for scenarios where the sourcing is moderate maximizes the chance of finding scenarios that produce large non-Gaussianity.…”
Section: Conditions For Large |Fnl|mentioning
confidence: 97%
“…And more likely than not, the sourcing will be moderate, but this is not a requirement. Rather, if the total sourcing is tiny (sin ∆ N ≪ 1) or is very large (cos ∆ N ≪ 1), then the trigonometric terms will make it even that much harder to satisfy the bound in equation (60). Figure 1 illustrates this point by showing the value of the factor sin 2 ∆ N cos 2 ∆ N as a function of the total mode sourcing, T RS .…”
Section: A Calculation Of Fnl Using the δN Formalismmentioning
confidence: 99%
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“…These consist of models in which both fields evolve during inflation, leading to a wide spectrum of possible behaviour [8][9][10][11][12][13][14][15][16][17][18]; curvaton-type behaviour which we define as the case where a second field begins to oscillate after the first field has reheated into radiation and its relative contribution to the energy density can gradually increase 2 [19][20][21][22][23][24][25] (also see Ref. [26,27]); and finally scenarios in which the process by which one (or both) of the fields reheat is directly dependent on the value of one of the light fields, which includes the scenarios known as Modulated Reheating (mr) [28][29][30][31][32][33][34][35] and the Inhomogeneous End of Inflation (iei) [36][37][38][39][40][41][42]. For reviews of these scenarios see Refs.…”
Section: Introductionmentioning
confidence: 99%
“…depends not only on the inflaton but also on another light field σ, the critical value φ cr also fluctuates, which leads to the perturbation of the duration of the inflation, that is, δN [29][30][31][32][33].…”
Section: Inhomogeneous End Of Hybrid Inflationmentioning
confidence: 99%